This document discusses the concepts of electrostatics including electric field, electric field intensity, electric field due to point charges, the superposition principle, electric lines of force, properties of electric lines of force, electric dipoles, electric field intensity due to dipoles, torque on dipoles, and work done on dipoles. It defines key terms and concepts and provides examples and equations to illustrate electric field and force calculations for various charge configurations including point charges and dipoles.

1. ELECTROSTATICS - II : Electric Field
By Arvind Kumar Physics Faculty at PW Patna
1. Electric Field
2. Electric Field Intensity or Electric Field Strength
3. Electric Field Intensity due to a Point Charge
4. Superposition Principle
5. Electric Lines of Force
i) Due to a Point Charge
ii) Due to a Dipole
iii) Due to a Equal and Like Charges
iv) Due to a Uniform Field
6. Properties of Electric Lines of Force
7. Electric Dipole
8. Electric Field Intensity due to an Electric Dipole
9. Torque on an Electric Dipole
10.Work Done on an Electric Dipole

2. Electric Field:
Electric field is a region of space around a charge or a system of charges
within which other charged particles experience electrostatic forces.
Theoretically, electric field extends upto infinity but practically it is limited to a
certain distance.
Electric Field Strength or Electric Field Intensity or Electric Field:
Electric field strength at a point in an electric field is the electrostatic force per
unit positive charge acting on a vanishingly small positive test charge placed
at that point.
E =
∆q
F
Lt
∆q → 0 q0
F
E =
The test charge is considered to be vanishingly small because its presence
should not alter the configuration of the charge(s) and thus the electric field
which is intended to be measured.
or or
q
r2
1
4πε0
E = r
+ q0 + q0
+ q - q
q – Source charge, q0 – Test charge, F – Force & E - Field
F
F

3. Note:
1. Since q0 is taken positive, the direction of electric field ( E ) is along the
direction of electrostatic force ( F ).
2. Electrostatic force on a negatively charged particle will be opposite to the
direction of electric field.
3. Electric field is a vector quantity whose magnitude and direction are
uniquely determined at every point in the field.
4. SI unit of electric field is newton / coulomb ( N C-1 ).

4. Electric Field due to a Point Charge:
O
Z
Y
X
+ q0
+ q
F
r
Force exerted on q0 by q is
q q0
r2
1
4πε0
r
F =
q q0
r3
1
4πε0
r
F =
P (x,y,z)
Electric field strength is
q0
F
E =
q
r3
1
4πε0
E (r) = r
or
or
r2
1
4πε0
E (r) =
q
r
The electric field due to a point charge has
spherical symmetry.
If q > 0, then the field is radially outwards.
If q < 0, then the field is radially inwards.
E
r2
0

5. Electric field in terms of co-ordinates is given by
( x2 + y2 + z2 ) 3/2
1
4πε0
E (r) =
q
i j k
( x + y + z )
Superposition Principle:
+ q2
- q3
- q5
+ q4
+ q1
F12
F14
F15
F13
The electrostatic force experienced by a
charge due to other charges is the vector
sum of electrostatic forces due to these
other charges as if they are existing
individually.
F1 = F12 + F13 + F14 + F15
F12
F14
F15
F13
F1
qa qb
1
4πε0
Fa (ra) = ∑
b=1
b≠a
N
ra - rb
ra - rb
│ │3
In the present example, a = 1 and b = 2 to 5.
If the force is to be found on 2nd charge,
then a = 2 and b = 1 and 3 to 5.

6. Superposition principle holds good for electric field also.
Note:
The interactions must be on the charge which is to be studied due to other
charges.
The charge on which the influence due to other charges is to be found is
assumed to be floating charge and others are rigidly fixed.
For eg. 1st charge (floating) is repelled away by q2 and q4 and attracted towards
q3 and q5.
The interactions between the other charges (among themselves) must be
ignored. i.e. F23, F24, F25, F34, F35 and F45 are ignored.
Electric Lines of Force:
An electric line of force is an imaginary straight or curved path along which a
unit positive charge is supposed to move when free to do so in an electric
field.
Electric lines of force do not physically exist but they represent real situations.
Electric Lines of Force
E
E

7. 1. Electric Lines of Force due to a Point Charge:
q < 0
q > 0
a) Representation
of electric field
in terms of
field vectors:
The size of the
arrow
represents the
strength of
electric field.
b) Representation
of electric field
in terms of
field lines
(Easy way of
drawing)

8. 2. Electric Lines of Force due to a
pair of Equal and Unlike Charges:
(Dipole)
+ q
- q
P
E
+ q
+ q
3. Electric Lines of Force due to a
pair of Equal and Like Charges:
.N
Electric lines of force contract
lengthwise to represent attraction
between two unlike charges.
Electric lines of force exert lateral
(sideways) pressure to represent
repulsion between two like charges.

9. 4. Electric Lines of Force due to a Uniform Field:
+
+
+
+
-
-
-
-
E
Properties of Electric Lines of Force
or Field Lines:
1. The electric lines of force are imaginary lines.
2. A unit positive charge placed in the electric field tends to follow a path
along the field line if it is free to do so.
3. The electric lines of force emanate from a positive charge and terminate on
a negative charge.
4. The tangent to an electric field line at any point
gives the direction of the electric field at that point.
5. Two electric lines of force can never cross each
other. If they do, then at the point of
intersection, there will be two tangents. It
means there are two values of the electric field
at that point, which is not possible.
Further, electric field being a vector quantity,
there can be only one resultant field at the
given point, represented by one tangent at the
given point for the given line of force.
E1
E2
E
+1 C
E
.
P

10. 6. Electric lines of force are closer
(crowded) where the electric field
is stronger and the lines spread
out where the electric field is
weaker.
7. Electric lines of force are
perpendicular to the surface of a
positively or negatively charged
body.
Q > q
q
Q
8. Electric lines of force contract lengthwise to represent attraction between
two unlike charges.
9. Electric lines of force exert lateral (sideways) pressure to represent
repulsion between two like charges.

11. 10.The number of lines per unit cross – sectional area perpendicular to the
field lines (i.e. density of lines of force) is directly proportional to the
magnitude of the intensity of electric field in that region.
11. Electric lines of force do not pass through a conductor. Hence, the interior
of the conductor is free from the influence of the electric field.
Solid or hollow
conductor
No Field
+
+
+
+
+
+
+
-
-
-
-
-
-
-
+
+
+
+
E E
-
-
-
-
α E
∆N
∆A
12. Electric lines of force can pass through an insulator.
(Electrostatic Shielding)

12. Electric Dipole:
Electric dipole is a pair of equal and opposite charges separated by a very
small distance.
The electric field produced by a dipole is known as dipole field.
Electric dipole moment is a vector quantity used to measure the strength of an
electric dipole.
+ q
- q
2 l
p
p = (q x 2l) l
The magnitude of electric dipole moment is the product of magnitude of either
charge and the distance between the two charges.
The direction is from negative to positive charge.
The SI unit of ‘p’ is ‘coulomb metre (C m)’.
Note:
An ideal dipole is the dipole in which the charge becomes larger and larger
and the separation becomes smaller and smaller.

13. Electric Field Intensity due to an Electric Dipole:
i) At a point on the axial line:
Resultant electric field intensity
at the point P is
EP = EA + EB
The vectors EA and EB are
collinear and opposite.
1
4πε0
i
EA =
q
(x + l)2
q
(x - l)2
1
4πε0
i
EB =
│EP │ = │EB│ - │EA│
│EP │ =
q
(x + l)2
q
(x - l)2
1
4πε0
]
[ -
│EP │ =
1
4πε0
2 (q . 2l) x
(x2 – l2)2
│EP │ =
1
4πε0
2 p x
(x2 – l2)2
If l << x, then
EP ≈
2 p
4πε0 x3
The direction of electric field intensity
at a point on the axial line due to a
dipole is always along the direction of
the dipole moment.
l
l
x
P
EP = EB - EA
+ q
- q
p
A B EA EB
O
EP =
1
4πε0
2 p x
(x2 – l2)2
i

14. θ
θ
l
l
y
θ
θ
+ q
- q
p
A B
EB
EA
EQ Q
Resultant electric field intensity
at the point Q is
EQ = EA + EB
The vectors EA and EB are
acting at an angle 2θ.
ii) At a point on the equatorial line:
q
( x2 + l2 )
1
4πε0
EA = i
q
1
4πε0
EB = i
( x2 + l2 )
EB
EA
EQ
θ
θ
EA cos θ
EB cos θ
EB sin θ
EA sin θ
The vectors EA sin θ and EB sin θ
are opposite to each other and
hence cancel out.
The vectors EA cos θ and EB cos θ
are acting along the same direction
and hence add up.
EQ = EA cos θ + EB cos θ
EQ =
q
2
4πε0 ( x2 + l2 )
l
( x2 + l2 )½
1
EQ =
4πε0
q . 2l
( x2 + l2 )3/2
EQ =
1
4πε0
p
( x2 + l2 )3/2
Q
O

15. EQ =
1
4πε0
p
( x2 + l2 )3/2
(- i )
If l << y, then
EQ ≈
p
4πε0 y3
The direction of electric field intensity at a point on the equatorial line due to a
dipole is parallel and opposite to the direction of the dipole moment.
If the observation point is far away or when the dipole is very short, then the
electric field intensity at a point on the axial line is double the electric field
intensity at a point on the equatorial line.
i.e. If l << x and l << y, then EP = 2 EQ

16. Torque on an Electric Dipole in a Uniform Electric Field:
The forces of magnitude pE act
opposite to each other and hence net
force acting on the dipole due to
external uniform electric field is zero.
So, there is no translational motion of
the dipole.
θ
However the forces are along different
lines of action and constitute a couple.
Hence the dipole will rotate and
experience torque.
Torque = Electric Force x distance
θ
t = q E (2l sin θ)
= p E sin θ
q E
q E
+ q
- q
E
2l
t
p
E
Direction of Torque is perpendicular
and into the plane containing p and E.
SI unit of torque is newton metre (Nm).
Case i: If θ = 0°, then t = 0.
Case ii: If θ = 90°, then t = pE
(maximum value).
Case iii: If θ = 180°, then t = 0.
t = p x E
p

17. Work done on an Electric Dipole in Uniform Electric Field:
dW = tdθ
= p E sin θ dθ
W = ∫ p E sin θ dθ
W = p E (cosθ1 - cos θ2)
θ1
θ2
If Potential Energy is arbitrarily taken zero when the dipole is at 90°,
then P.E in rotating the dipole and inclining it at an angle θ is
Potential Energy U = - p E cos θ
Note: Potential Energy can be taken zero arbitrarily at any position of the
dipole.
- q
2l
q E
E
θ1 θ2
+ q
q E
q E
q E
When an electric dipole is placed in a uniform electric field, it experiences
torque and tends to allign in such a way to attain stable equilibrium.
Case i: If θ = 0°, then U = - pE (Stable Equilibrium)
Case ii: If θ = 90°, then U = 0
Case iii: If θ = 180°, then U = pE (Unstable Equilibrium)
dθ
END